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Dual Nature of Radiation and Matter Test - 12

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Dual Nature of Radiation and Matter Test - 12
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  • Question 1
    1 / -0
    The de Broglie wavelength of an electron in the $$4^{th}$$ Bohr orbit is:
    Solution
    De-Broglie wavelength of an electron:
     
    $$2\pi r = n\lambda$$

    $$2\pi \times \dfrac{n^2}{z} a_0 = n.\lambda$$

    $$2\pi \times \dfrac{4^2}{1}a_0 = 4\lambda$$

    $$\lambda = 8\pi a_0$$

    Hence, the correct answer is option $$C$$.
  • Question 2
    1 / -0
    If the de Broglie wavelengths associated with a proton and an $$\alpha -$$ particle are equal, then the ratio of velocities of the proton and the $$\alpha -$$ particle will be:
    Solution
    Given de Broglie Wavelength $$ \lambda_{p} = \lambda_{\alpha}$$

    So, $$\dfrac {h}{m_{p} \times v_{p}}$$ = $$\dfrac {h}{m_{\alpha} \times v_{\alpha}}$$

    $$\dfrac{v_{p}} {v_{\alpha}}$$ = $$ \dfrac {m_{\alpha}}{m_{p}}$$ = $$\dfrac{4 m_{p}} {m_{p}}$$

    Because Mass of $$\alpha$$ particle is 4 times mass of proton.

    So 4:1. 

    Option C is correct answer
  • Question 3
    1 / -0
    An electron (of mass m) and a photon have the same energy E in the range of a few eV. The ratio of the de-Broglie wavelength associated with the electron and the wavelength of the photon is (c = speed of light in vacuum)
    Solution
    For electron
    De - Broglie wavelength $$\lambda_c = \dfrac{h}{p}$$
    where p is momentum $$p = mv$$
    also by energy we have $$E = \dfrac{1}{2} mv^2$$

    $$\Rightarrow E = \dfrac{1}{2} \dfrac{p^2}{m}$$

    $$\Rightarrow p = \sqrt{2 mE}$$

    $$\therefore \lambda_c = \dfrac{h}{\sqrt{2 mE}}$$

    For photon energy $$\Rightarrow E = \dfrac{hc}{\lambda}$$

    $$\Rightarrow \lambda = \dfrac{h c}{E}$$

    $$\therefore \dfrac{\lambda_c}{\lambda} = \dfrac{h}{\sqrt{2 mE}} \dfrac{E}{hc}$$

    $$= \dfrac{1}{C} \sqrt{\dfrac{E}{2m}}$$

    option (A) is correct.
  • Question 4
    1 / -0
    A particle moving with kinetic energy E has de Broglie wavelength $$\lambda$$. If energy $$\Delta E$$ is added to its energy, the wavelength become $$\lambda /2$$. Value of $$\Delta E$$, is?
    Solution
    For Partial,

    $$\lambda=\dfrac{h}{\sqrt{2\times (K.E)\times m}}$$

    $$\lambda \propto \dfrac{1}{\sqrt{K.E}}$$

    $$\dfrac{\lambda_1}{\lambda_2}=\sqrt{\dfrac{(K.E)_2}{(K.E)_1}}=\sqrt{\left(\dfrac{E+\Delta E}{E}\right)}$$

    $$\left(\dfrac{\lambda}{\lambda/2}\right)^2=\dfrac{E+\Delta E}{E}$$

    $$4=1+\dfrac{\Delta E}{E}$$

    $$3=\dfrac{\Delta E}{E}$$

    $$\boxed{\Delta E=3E}$$

    Option (C) is correct.
  • Question 5
    1 / -0
    The relative uncertainty in the period of a satellite orbiting around the earth is $$10^{-2}$$. If the relative uncertainty in the radius of the orbit is negligible, the relative uncertainty in the mass of the earth is :
    Solution
    Time period, $$T = 2 \pi \sqrt{\dfrac{r^3}{GM_e}}$$

    Squaring om both sides, $$T^2 = \dfrac{4 (\pi)^2 r^3}{GM}$$

    Taking log, $$ln(T^2)= ln(\dfrac{4 (\pi)^2 r^3}{GM})$$

    $$ln(T^2) = ln(\dfrac{4 (\pi)^2 r^3}{G})-ln(M)$$

    $$2 ln(T) = ln(K)-ln(M)$$

    $$2 \dfrac{\Delta{T}}{T}= \dfrac{\Delta{M}}{M}$$

    $$\dfrac{\Delta{M}}{M}= 2 \times 10^{-2}$$
  • Question 6
    1 / -0
    An electron of mass $$m$$ and magnitude of charge $$|e|$$ initially at rest gets accelerated by a constant electric field $$E$$. The rate of change of de-Broglie wavelength of this electron at time $$t$$ ignoring relativistic effects is:
    Solution
    $$P=\dfrac{h}{\lambda_D}$$

    $$\lambda_D=\dfrac{h}{p}=\dfrac{h}{mv}$$

    $$\because \dfrac{v}{t}=a\Rightarrow v=at$$

    $$v=at$$

    $$\because F=qE$$

    $$ma=qE$$

    $$\boxed{a=\dfrac{qE}{m}=\dfrac{eE}{m}}$$

    So, $$v=\dfrac{|e|E}{m}t$$

    $$\therefore \lambda_D=\dfrac{h}{m\left(\dfrac{|e|E}{m}\right)t}=\dfrac{h}{|e|Et}$$

    Rate of change of de-Broglie wavelength is given by differentiating the wavelength w.r.t. time.
    $$\boxed{\dfrac{d\lambda_D}{dt}=-\dfrac{h}{|e|Et^2}}$$
  • Question 7
    1 / -0

    A proton has kinetic energy $$\mathrm{E}=100\mathrm{k}\mathrm{e}\mathrm{V}$$ which is equal to that of a photon. The wavelength of photon is $$\lambda_{2}$$ and that of proton is $$\lambda_{1}$$. The ratio of $$\lambda_{1}/\lambda_{2}$$ is proportional to
    Solution
    For proton and photon wavelength is given as -
    $$\displaystyle \lambda_{\mathrm{p}\mathrm{r}\mathrm{o}\mathrm{t}\mathrm{o}\mathrm{n}}=\frac{\mathrm{h}}{\sqrt{2\mathrm{m}\mathrm{E}}},\ \displaystyle \lambda_{\mathrm{p}\mathrm{h}\mathrm{o}\mathrm{t}\mathrm{o}\mathrm{n}}=\frac{\mathrm{h}\mathrm{c}}{\mathrm{E}}$$.
    So, the answer is option (B).
  • Question 8
    1 / -0
    A proton is fired from very far away towards a nucleus with charge Q = 120 e, where e is the electronic charge. It makes a closest approach of 10 fm to the nucleus. The de Broglie wavelength (in units of fm) of the proton at its start is :

     (take the proton mass, $$m_p = (5/3) \times 10^{-27}kg$$ and

    $$h/e = 4.2\times 10^{-15}J.s/C; \frac{1}{4\pi\epsilon_0} = 9 \times 10^9 m/F; 1 fm = 10^{-15}m$$)
    Solution

    Given here,

    $$q_{1} = 120 \times e$$

    $$q_{2} = e $$ ( charge on proton)

    It is based on conservation of energy of proton.

    $$\dfrac{1}{2}mv^2 = k \dfrac{q_1q_2}{R}$$

    $$v = \sqrt{\dfrac{2Kq_1q_2}{mR}}$$

    Also, we know, de’broglie wavelength,

    $$\lambda =\dfrac{h}{mv}$$

    $$\lambda = \dfrac{h\sqrt{R}}{\sqrt{2mKq_1q_2}}\\$$

    Thus,

    $$\lambda = \dfrac{h\sqrt{10\times10^{-15}}}{\sqrt{2\times\dfrac{5}{3}\times10^{-27}\times9\times10^9\times120\times e^2}}\\$$

    $$\lambda =\dfrac{\dfrac{h}{e}\times10^{-7}}{6\times10^{-8}}\\$$

    $$\lambda =\dfrac{4.2\times10^{-15}\times10^{-7}}{6\times10^{-8}}\\$$

     $$\lambda =7\times10^{-15}\ m = 7\ fm \\$$

    Option A is correct.

  • Question 9
    1 / -0
    A pulse of light of duration 100 ns is absorbed completely by a small object initially at rest. Power of the pulse is 30$$mW$$and the speed of light is $$3\times 10^{8}m/s$$. The final momentum of the object is:
    Solution
    Sol$$. (B)$$
    $$t=100\times 10^{-9} sec,\ P=30\times 10^{-3}$$Watt, 
    $$C=3\times 10^{8}m/s$$
    Incident energy $$= Pt$$
    By debroglie wavelength, $$\lambda=h/p$$
    and Energy of photon is $$E=hc/\lambda$$
    From above two equations, $$E=pc$$ 

    Momentum $$p=\dfrac{Pt}{C}=\dfrac{30\times 10^{-3}\times 100\times 10^{-9}}{3\times 10^{8}}=1.0\times 10^{-17}$$ kg ms$$^{-1} $$

    So, the answer is option (B).
  • Question 10
    1 / -0

    Directions For Questions

    When a particle is restricted to move along x-axis between $$x = 0$$ and $$x = a$$, where a is of nanometer dimension, its energy can take only certain specific values. The allowed energies of the particle moving in such a restricted region,correspond to the formation of standing waves with nodes at its ends $$x=0$$ and $$x=a$$. The wavelength of this standing wave is related to the linear momentum p of the particle according to the de Broglie relation. The energy of the particle of mass m is related to its linear momentum as $$E = p^{2}/2m$$. Thus, the energy of the particle can be denoted by a quantum number n taking values $$1, 2, 3, . $$($$n = 1$$, called the ground state) corresponding to the number of loops in the standing wave.
    Use the model described above to answer the following three questions for a particle moving in the line $$x = 0$$ to $$x = a$$. Take $$h = 6.6 \times 10^{-34} Js$$ and $$e = 1.6 \times 10^{-19} C.$$

    ...view full instructions

    The speed of the particle that can take discrete values is proportional to
    Solution
    As given in the question
    Let the no. of loops in the wave be  $$n$$
    Let wavelength be $$\lambda$$ 
    Debroglie wavelength
    $$ \lambda = \cfrac{h}{mv}$$ ------------(1)
    Also
    $$ n \lambda = 2 \pi a$$  --------------(2)
    Substituting above
    $$ v = \cfrac{nh}{2am}$$
    $$v \propto n$$
    So, the answer is option (D).
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